whatif said:
That corresponds to a yes to my first question.
No, it doesn't. The timelike
basis vector points into the future. That doesn't mean the
energy points into the future. You could say that the vector you get when you multiply the energy times the timelike basis vector points into the future, but that vector is not the energy. Energy doesn't have a direction, and "the direction of time" (i.e., "into the future") is not the energy, or the direction of the energy.
whatif said:
mass (rest mass) is invariant between frames
Yes.
whatif said:
spatial velocities can be transformed so that momentum (spatial component) can be transformed
Not by themselves; you have to transform all four components of a 4-vector together. See further comments below.
whatif said:
time always points in the same direction
No, it doesn't. More precisely, the timelike basis vector doesn't always point in the same direction. Nor do the spatial ones. It might help to work through this in more detail.
In ordinary Cartesian coordinates in ordinary 3-dimensional space, you can rotate the coordinates, which changes the directions in which the basis vectors point. The components of all vectors change when you transform them from one set of coordinates to the other.
In 4-dimensional spacetime, a Lorentz transformation--a change of inertial frames--works similarly: it changes the directions in which the basis vectors point. But now we have to include the timelike basis vector in this; in other words, changing inertial frames changes which way the timelike basis vector points, as well as the spatial ones. Actually, a pure Lorentz transformation--what you'll often see called a "boost" in the literature--only changes the direction in spacetime of one spatial vector, the one that points in the direction of relative motion between the two frames.
But there is a key difference, intuitively speaking, with a Lorentz transformation. Note that I said above "direction in spacetime",
not "direction in space". A pure boost does not "mix" directions in space: it only changes the direction in spacetime of one spatial basis vector, leaving the other two spatial basis vectors alone. But it also changes the direction in spacetime of the timelike basis vector. You can see an illustration of how this works here:
https://en.wikipedia.org/wiki/Minkowski_diagram#Minkowski_diagrams_in_special_relativity
If you look at the first diagram on the right in that section of the article, the black axes are the ##t## and ##x## axes (the ##x## direction is the direction of relative motion) before the transformation, and the blue axes are after the transformation. Note that the axes "tilt" towards each other, instead of staying at 90 degrees in the diagram as a normal spatial rotation would do. That's because the geometry of spacetime is not Euclidean, it's Minkowskian (the minus sign in the metric). But the point is that both axes change direction in spacetime (spacetime here is just the diagram as a whole) in the transformation, so both the ##t## and the ##x## components of vectors have to change.
whatif said:
so that energy can, in principle, be treated as a scalar quantity
The term "scalar quantity" is ambiguous. Strictly speaking, a "scalar" in relativity (more precisely, a "Lorentz scalar") is a quantity that's just a number (no direction) and doesn't change when you change frames. So rest mass is a scalar, on this strict definition, but energy is not. Energy is just one component of a 4-vector, and transforms like all vector components when you change frames.